2.1. Synergistic UV/TiO2/IO4− Treatment
The photocatalytic degradation of SO (10 mg/L) was investigated using TiO
2 (0.4 g/L) in the presence of IO
4− ions (0.15 mM) under UV irradiation at pH 6. Preliminary tests were performed under IO
4− alone, TiO
2/IO
4−, UV/IO
4−, and classical photocatalysis (UV/TiO
2) conditions to assess the contribution of each component. The resulting concentration–time data were analyzed using the pseudo-first-order kinetic model, which provides a quantitative means of determining the apparent rate constants for the different reaction systems (
Figure 1). Residual analysis confirmed that deviations from the pseudo-first-order model were random and exhibited no systematic trends, thereby supporting the validity of the applied kinetic treatment. The complete concentration–time profiles have been published in the earlier study [
3]. Across all conditions, including elevated scavenger concentrations, no departure from pseudo-first-order behavior was detected. The coefficients of determination (R
2) for the kinetic fits consistently exceeded 0.98, underscoring the robustness of the model and the reliability of the derived rate constants. The UV/TiO
2/IO
4− system exhibited a first-order rate constant dramatically larger than any binary combination. These results establish an unequivocal super-additive response when UV, TiO
2, and periodate act concurrently. Literature documents IO
4− as a conduction band electron acceptor that limits recombination and as a photochemically activatable precursor of iodine-centered oxidants and hydroxyl radicals in UV/TiO
2/IO
4− and related UV/IO
4− systems [
6,
13]. Evidence in this manuscript for operative oxidants, including interfacial holes, hydroxyl radicals, and an electron or superoxide branch, derives from the structured scavenger panel and the kinetic analyses described later. Interpretation integrates established aqueous radical rate constants and selectivity compendia with trends in inhibition strength and matrix dependence observed in this dataset, with explicit acknowledgment of caveats on scavenger selectivity in heterogeneous photocatalysis [
15,
16,
17]. The synergy ratio (SR
3) of the ternary system relative to the sum of the binary baselines was evaluated to quantify the interaction:
The calculated synergy ratio is 11.9.
To formalize the baseline, the ternary synergy based on an additive expectation is defined as SR3 equals the observed pseudo-first order rate constant in the ternary system divided by the sum of the pseudo-first order rate constants measured for the binary systems studied here. This baseline reflects independent, parallel oxidation channels and is the analog of Bliss additivity used to screen for supra-additive behavior. For completeness, a conservative single process benchmark is also reported as SRmax equals the observed pseudo-first order rate constant in the ternary system divided by the largest pseudo-first order rate constant among the binary systems. Because the sum in the denominator of SR3 is greater than or equal to the maximum term, SR3 is less than or equal to SRmax for the same dataset. Reporting both values prevents overinterpretation and enables comparison with the broader advanced oxidation literature, where some studies adopt the sum baseline while others reference the highest single binary process.
For comparison, the enhancement relative to the best binary processes is substantial, with SRmax1 = () ≈ 20.8 and SRmax2 = () ≈ 28.8. This demonstrates that three-way coupling offers significantly greater benefits than any two-component combination. This level of synergy is consistent with the well-established role of periodate in photo-TiO2 systems. IO4− acts as a conduction-band electron scavenger. This suppresses electron/hole recombination and increases the flux of valence-band holes, which form •OH radicals from surface H2O/OH−. This electron sink function is widely recognized as the primary means of achieving higher apparent rates in TiO2 photocatalysis. Additionally, UV activation of periodate and the reduction of IO4− by photogenerated electrons open iodine-centered radical and high-valent iodine pathways (e.g., IO4•, IO3•, and I2•−). These pathways complement •OH/O2•− chemistry, broadening the oxidative spectrum to include cationic dyes, such as SO. Moreover, combining UV/TiO2 with IO4− creates a redox shuttle (I(VII) ⇌ I(V)/I(III)), accelerating interfacial charge transfer and sustaining radical production.
Under UVA irradiation at 365 nm and pH 6 in the presence of TiO
2 and dissolved oxygen, IO
4− functions as an electron acceptor and photochemical oxidant. In this matrix, periodate activation yields iodine-centered radicals IO
3• and IO
4• together with reactive oxygen species, and concomitantly undergoes reduction to iodate, which accumulates as the stable iodine sink. Transient spectroscopy on iodate and periodate in water has identified short-lived iodine(VI) intermediates that connect iodine(VII) to lower oxidation states during irradiation, supporting cycling within the iodine redox manifold under aqueous photochemical conditions [
6,
18]. Reports of homogeneous and heterogeneous UV- or UVA-activated periodate at circumneutral pH corroborate these steps and the dominance of iodate as the product under oxic conditions [
18,
19,
20]. Iodine speciation was not resolved in this dataset. Reports on UV or photocatalytic periodate under oxic conditions identify iodate as the dominant product and document iodine-centered radicals and transient iodine intermediates, consistent with I(VII) to I(VI) to I(V) cycling under the used conditions [
13].
The UV/TiO
2/IO
4− system yielded a pseudo-first order rate coefficient of 0.6212 min
−1. Homogeneous UV–periodate systems on azo dyes report first-order fits with rate coefficients typically on the order of 10
−2 to 10
−1 min
−1 at comparable ultraviolet fields and millimolar periodate [
13]. Catalyst-activated periodate systems frequently report higher values; representative examples include values near 5 × 10
−1 min
−1 for pharmaceutical surrogates, subject to pollutant identity and matrix [
21]. These ranges place the present value at the upper end of periodate AOP performance, consistent with the dual role of periodate as an electron acceptor that suppresses recombination and as a photochemically activatable oxidant precursor.
The weak performance of IO4− alone and TiO2/IO4− in the dark is also mechanistically coherent. Without photons, there are no TiO2 e−/h+ pairs, and periodate lacks an efficient activation channel. Thus, only slow direct oxidation or limited background homolysis occurs. Upon UV illumination, both direct photoactivation of IO4− and photocatalytic routes become available and reinforce each other. This explains the order-of-magnitude increase in k for the ternary system.
To illustrate, the nearly 21-fold improvement compared with the most effective binary systems, together with an SR3 value of 11.9, demonstrates that the ternary configuration harnesses photons, the catalyst, and the oxidant in both an additive and synergistic fashion. This outcome highlights the UV/TiO2/IO4− process as an exceptionally powerful advanced oxidation pathway for SO degradation.
  2.2. Scavenger Impact
Understanding which oxidants and charge carriers govern SO degradation in the UV/TiO2/IO4− process is essential for mechanism-driven design. Seven mechanistic scavengers were employed to identify the dominant oxidant species within the UV/TiO2/IO4− process: ascorbic acid (AA), methanol (MeOH), benzoquinone (BQ), oxalate (OX), sodium dichromate (Na2Cr2O7), sodium azide (NaN3), and phenol (Ph).
To guide interpretation without over-committing to absolute energy placements, a concise band-centered narrative is adopted. Under pristine conditions, photoexcitation promotes electrons to the conduction band and creates holes in the valence band. Electrons reduce adsorbed oxygen to superoxide, and holes oxidize interfacial water or hydroxide to hydroxyl radicals, while band-to-band recombination remains a major loss channel. At intermediate additive levels where an electron acceptor is present, periodate traps conduction band electrons and forms iodine-centered oxidants, recombination is suppressed, and holes continue to generate hydroxyl radicals with modest competition from hole scavengers. At high additive levels, scavenging and trapping dominate, diverting both electrons and holes from productive routes, radical formation declines, and recombination regains prominence. This qualitative progression matches the measured trends and is consistent with the known pH-dependent and interface-sensitive positions of TiO2 band edges.
As illustrated in 
Figure 2, the inhibition patterns correspond to the expected redox and radical-scavenging chemistry of the UV/TiO
2/IO
4− system. Specifically, the rate of SO removal slows progressively as AA or MeOH is added. In the additive-free control, SO decays rapidly, reflecting the efficient separation of charges on TiO
2 and the rapid generation of reactive intermediates (
•OH, IO
3•, and IO
4•) from photoactivated periodate. These intermediates complement surface h
+/
•OH pathways.
Introducing AA results in strong, dose-dependent suppression (
Figure 2a). It should be noted that complete inhibition of SO degradation was already observed at 1 mM AA. The kinetic profile at this concentration was superposed with that obtained at 10 mM, indicating that the threshold for total quenching is reached at or below 1 mM. Three concurrent mechanisms explain this potency. First, the reactive ascorbate monoanion (AH
−) consumes 
•OH radicals at diffusion-controlled rates (k = 10
9–10
10 M
−1·s
−1 [
15]), diverting oxidants directly away from SO. Second, AA efficiently reduces photogenerated iodine radicals and oxidants from IO
4− photolysis. This short-circuits the intended IO
7−/IO
4−/IO
3− redox cycling. This erodes the electron-acceptor role of periodate, which normally suppresses e
−/h
+ recombination. Third, AA behaves as a fast hole/electron transfer substrate at illuminated TiO
2, competing with SO for photogenerated holes and reducing the dye’s accessible oxidizing capacity. Together, these pathways explain why submillimolar AA decelerates SO degradation and why 1 mM AA largely quenches the process.
MeOH inhibits SO degradation in a clear, monotonic fashion, albeit less dramatically than AA at the same molarity (
Figure 2b). This difference is mechanistically reasonable. MeOH is a well-known 
•OH and hole scavenger. It reacts with 
•OH with a reaction rate constant of (9–10) × 10
8 M
−1·s
−1 [
15]. These reactions remove oxidizing equivalents from SO and reduce the effective radical/charge density near the semiconductor interface. Unlike AA, however, methanol does not strongly reduce iodine intermediates or periodate itself. Therefore, ternary synergy is primarily weakened by radical and hole quenching rather than by the collapse of the IO
4− electron-acceptor cycle. This explains the milder inhibition at equal concentrations.
Viewed as a whole, the data emphasize that the remarkable performance of UV/TiO2/IO4− relies on three factors: access of SO to illuminated TiO2 surfaces, the rapid scavenging of photogenerated electrons by IO4−, and an undisturbed radical inventory from IO4− photolysis.
Adding either BQ or OX suppresses SO removal, and this inhibition is clearly dose-dependent (
Figure 3). In the BQ series, concentrations of 0.01–0.1 mM result in modest slowing. However, concentrations of 1–10 mM leave a significant amount of residual SO after 50 min. This pattern aligns with 
p-BQ’s established role as a superoxide (O
2•−) scavenger and electron acceptor in photocatalytic systems. BQ intercepts conduction-band electrons and O
2•−, thereby diminishing the O
2•−-pathway and the associated downstream oxidants (e.g., H
2O
2/
•OH). These oxidants normally complement hole/
•OH chemistry in TiO
2 photocatalysis. Thus, the observed deceleration occurs. Note that BQ reacts rapidly with 
•OH (k = 6.6 × 10
9 M
−1·s
−1 [
15]). Therefore, at mM doses, BQ competes with the dye for hydroxyl radicals and reduces the available oxidant. Together, these mechanisms provide a basis for the strong, monotonic inhibition observed. However, BQ can undergo side photochemistry (e.g., photogenerated 
1O
2 or altered 
•OH formation) and may not be perfectly selective for O
2•− under UV conditions. Nevertheless, the results in 
Figure 3 show consistent suppression across the full BQ range. Under the present conditions (UV/TiO
2/IO
4−, pH 6), the net effect is inhibitory. This finding supports the meaningful contribution of O
2•−/electron-mediated steps in the ternary process.
Similarly, OX impedes SO degradation (
Figure 3b). It has minimal effects at 0.1 mM but substantially inhibits degradation at 10–100 mM. As a classic hole scavenger, oxalate binds to TiO
2 and undergoes photodecarboxylation [
22,
23,
24]. This process consumes valence-band holes, thereby reducing the formation of 
•OH at the interface. It also competes with dye oxidation. Strong adsorption near the TiO
2 point of zero charge can block reactive sites, thereby reducing the reaction rate at higher concentrations.
In the context of the UV/TiO2/IO4− mechanism, these scavenger tests reinforce the cooperative roles of holes, •OH, and electron-derived species. Periodate typically acts as an efficient electron acceptor, suppressing e−/h+ recombination and participating in iodine-centered radical chemistry. The introduction of BQ competes for those electrons and removes superoxide anion radicals, while OX removes holes before they can oxidize surface water or adsorbates. The net result is slower SO removal in both series, highlighting that both charge-carrier channels are operative and disruption of either channel degrades performance.
Figure 4a shows that Cr
2O
72− markedly inhibits SO degradation, with stronger inhibition occurring at higher concentrations (0.1 mM, 1 mM, and 10 mM, in that order). In contrast, azide produces only a slight and nearly negligible slowdown at these concentrations (
Figure 4b). These contrasting behaviors are consistent with the distinct roles of the two additives in photoinduced redox and radical chemistry.
 Three effects act together for Cr2O72−. First, Cr2O72− strongly absorbs in the near-UV range (notably around 257 and 350 nm), creating an inner filter that reduces the number of photons reaching TiO2 and periodate. This optical penalty increases with concentration. Second, Cr2O72− is a potent electron acceptor at TiO2, forming surface complexes that are photoreduced to Cr(III). The resulting Cr(III) hydroxide/oxide deposits and related surface species are known to passivate active sites and promote recombination, progressively deactivating the photocatalyst. Third, in the UV/TiO2/IO4− system specifically, periodate functions as the intended electron sink and source of iodine-centered and •OH oxidants under UV light. However, introducing a competing electron acceptor (Cr2O72−) diverts electrons away from the reduction/activation of periodate. This weakens the synergy that normally accelerates dye removal. Under different conditions, Cr2O72− can promote photocatalysis by pairing electron consumption with hole-driven oxidation of organics. However, the present data show the opposite, likely because optical screening and surface deactivation outweigh the benefits of charge separation at pH 6 and the tested concentrations.
The minimal impact of N
3− suggests that singlet oxygen (
1O
2) likely plays a minor role in the removal of SO. Azide is a classic quencher of singlet oxygen, with rate constants ranging from 10
8 to 10
9 M
−1·s
−1 [
15]. If singlet oxygen were a dominant oxidant, strong inhibition would be evident. Additionally, azide reacts with 
•OH to form the azidyl radical (N
3•), which oxidizes aromatics. This reaction pathway can partially compensate for 
•OH scavenging and help explain the weak net effect observed.
Collectively, these scavenger tests reinforce the idea that the impressive performance of UV/TiO2/IO4− hinges on maintaining photon delivery to TiO2, preserving periodate-mediated electron scavenging and radical formation, and avoiding surface passivation. Strongly absorbing/electron-accepting species, such as Cr2O72−, undermine these requirements (optical filtering, site blocking, and competition for electrons). However, azide’s quenching of 1O2 is largely irrelevant because 1O2 contributes minimally under these conditions.
Ph clearly inhibits SO degradation in a concentration-dependent manner (
Figure 5). A concentration as low as 0.01 mM slows decay, while a concentration between 0.1 and 1.0 mM results in significant kinetic penalties. A concentration of 10 mM leaves a substantial residual after 50 min. This behavior is consistent with Ph’s well-documented reactivity toward oxidizing species and charge carriers that drive the UV/TiO
2/IO
4− process. Ph is an exceptionally fast scavenger of 
•OH in water, with a typical k = 10
9–10
10 M
−1·s
−1 [
15]. Thus, increasing Ph directly diverts hydroxyl radicals away from SO. Additionally, at pH 6, Ph is neutral (pKa = 10) and adsorbs onto TiO
2 near its point of zero charge, where surface complexation and hydrogen bonding are favored. This adsorption competitively blocks catalytic sites and limits SO’s access to photogenerated holes, which are prerequisites for rapid photocatalytic oxidation. In addition, Ph acts as an efficient hole scavenger on illuminated TiO
2; the rapid oxidation of Ph to phenoxyl/semiquinone radicals competes with dye oxidation. This reduces the effective hole flux available to initiate surface 
•OH and direct electron-transfer reactions. These inhibitory pathways are essential to the UV/TiO
2/IO
4− system because IO
4− scavenges conduction-band electrons. This process suppresses recombination and generates iodine-centered oxidants and 
•OH upon photoactivation. However, Ph erodes these three advantages by consuming 
•OH, competing for holes, and occupying TiO
2 surface sites. This explains the strong, monotonic slowdown in SO removal as Ph concentrations increase.
In summary, scavenger tests demonstrate that SO removal in the UV/TiO2/IO4− process depends on the presence of interfacial holes, •OH radicals, and electron-driven pathways. The strong inhibition by AA and Ph suggests rapid •OH (and hole) quenching and competitive interfacial electron transfer. Meanwhile, MeOH produces a milder slowdown, consistent with its role as a •OH/hole scavenger. The pronounced effects of BQ and OX highlight the importance of the e−/O2•− branch and valence-band holes, respectively. BQ intercepts conduction-band electrons and O2•−, and OX acts as a classic TiO2 hole scavenger. Cr2O72− suppresses performance optically due to strong UV absorption and inner filtering, as well as kinetically by competing for electrons. This undermines the periodate-assisted charge separation that drives the ternary synergy. In contrast, azide has little impact, suggesting that 1O2 is, at most, a minor contributor under these conditions, despite azide’s high quenching rate for singlet oxygen.
Selectivity limits of the scavenger panel warrant clarification. BQ intercepts conduction band electrons and superoxide, yet also reacts rapidly with hydroxyl radicals in water, with a reported second-order rate constant of 6.6 × 109 M−1·s−1. Therefore, inhibition by BQ reflects joint interception of electrons, superoxide, and hydroxyl radicals. Ph and MeOH each remove hydroxyl radicals and also consume photogenerated holes at the TiO2 surface, which complicates assignment based on a single quencher. Under these conditions, interpretation benefits from orthogonal diagnostics. EPR with spin trapping can be used to confirm the presence of radical intermediates, including superoxide adducts that are stabilized by traps such as 5-(diethoxyphosphoryl)-5-methyl-1-pyrroline N-oxide (DEPMPO) or 5-(diisopropoxyphosphoryl)-5-methyl-1-pyrroline N-oxide (DIPPMPO). Independent singlet oxygen readout can be obtained from furfuryl alcohol loss or from the conversion of 2,2,6,6-tetramethylpiperidine (TEMP) to 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO) with appropriate controls. The combined approach reduces misattribution and supports the conclusion that holes and hydroxyl radicals are the predominant oxidants, while the electron and superoxide branches serve as contributory pathways.
The inference of iodine-centered radicals from scavenger outcomes and matrix effects is consistent with direct observations reported for periodate systems. In UV/TiO
2/IO
4−, EPR with 5,5-dimethyl-1-pyrroline N-oxide (DMPO) shows hydroxyl and superoxide signals in agreement with the probe trends, supporting a mixed oxidant pool in this photocatalytic matrix [
6]. In ozone activated periodate, EPR resolves an iodate radical and confirms concurrent reactive oxygen species, demonstrating that iodine species can be captured by spin trapping under aqueous conditions [
25]. Transient spectroscopic studies on photoactivated periodate further identify short lived iodine intermediates that connect periodate to lower iodine oxidation states, which is compatible with the proposed pathway [
20].
  2.4. Salt Impact
Figure 7a shows how chloride affects SO removal in the UV/TiO
2/IO
4− process. As the NaCl concentration increases from 0.1 to 100 mM, SO decay progressively slows. This is consistent with three chloride-driven effects. First, chloride converts 
•OH into reactive chlorine species (RCS) through rapid reactions yielding Cl
2•−/ClOH
•−. These RCS are longer-lived; however, they react with organics much more slowly than 
•OH. Typical k
Cl2•− values range from 10
5 to 10
8 M
−1·s
−1 [
26], whereas k
•OH values range from 10
9 to 10
10 M
−1·s
−1 [
15]. This reduces the effective oxidant strength experienced by SO. Second, chloride competes with photogenerated holes on illuminated TiO
2 and blocks adsorption sites. This lowers interfacial 
•OH formation and hinders dye access to reactive centers. Third, photocatalytic rates decrease further at higher salinity levels due to a reduction in active surface area, as well as an alteration of the double layer caused by increased ionic strength, TiO
2 aggregation, and anion coverage.
 The UV/TiO2/IO4− process relies on fast hole/•OH chemistry at the TiO2 interface, periodate-mediated electron scavenging, and multi-radical generation. The shift from •OH to the less reactive RCS, coupled with surface and site effects, explains the consistent decline in performance in the presence of chloride. Some removal persists at moderate chloride concentrations due to the residual activity of RCS and non-radical pathways. However, the net influence is clearly inhibitory.
Figure 7b shows that increasing the concentration of Na
2SO
4 from 0.1 to 100 mM progressively slows the decay of SO. This suggests that sulfate interferes with both interfacial charge transfer and oxidant availability. Sulfate competitively consumes 
•OH to form SO
4•− (
•OH + SO
42− → SO
4•− + OH
−) [
16]. For the aqueous matrices examined, the reaction of hydroxyl radical with sulfate is not expected to be a controlling sink. Using a representative second-order rate constant of about 1.2 × 10
7 M
−1·s
−1 and a sulfate level of approximately 28–30 mM in seawater, the corresponding pseudo-first order loss rate is about 3.4–3.6 × 10
5 s
−1. In the same matrices, chloride attains about 0.5–0.6 M and reacts with the hydroxyl radical at 4.3 × 10
9 M
−1·s
−1, giving pseudo-first-order loss rates ≥2 × 10
9 s
−1. Consequently, the chloride pathway dominates hydroxyl radical scavenging by roughly four orders of magnitude, whereas conversion to sulfate radical via sulfate remains a minor channel under the conditions used. Since SO
4•− oxidizes aromatics more slowly than 
•OH, the radical pool becomes less effective as sulfate increases. In parallel, elevated ionic strength and the divalent character of SO
42− promote TiO
2 aggregation and compress the electrical double layer. These effects reduce accessible surface area and mass transfer. Additionally, sulfate can specifically adsorb onto metal oxide surfaces, altering surface charge and blocking reactive sites. This type of inner-/outer-sphere complexation is well-established on oxides and helps explain the rate losses observed. Together with the known sensitivity of TiO
2 photocatalysis to inorganic anions, these factors help explain the monotonic inhibition observed here. Sulfate shifts the system away from fast hole/
•OH-driven oxidation at illuminated TiO
2 toward less reactive pathways, simultaneously diminishing the effective catalytic surface area.
 Figure 8a shows that bicarbonate produced only a modest and gradual decrease in SO removal in the UV/TiO
2/IO
4− system at pH 8.3, even at concentrations up to 100 mM. This muted effect is mechanistically consistent with radical speciation and interfacial chemistry under these conditions. At pH 8.3, the carbonate system is dominated by HCO
3− (pK
1 = 6.35; pK
2 = 10.33). Thus, 
•OH is primarily diverted to the carbonate radical (CO
3•−) via the reaction 
•OH + HCO
3− (k = 10
7 M
−1·s
−1 [
15]) rather than being strongly quenched. CO
3•− is less reactive than 
•OH; however, it remains a competent and selective oxidant toward electron-rich aromatics (k typically 10
5–10
8 M
−1·s
−1 [
27]). This helps sustain dye decay. Surface processes further explain the resilience. At this pH, the TiO
2 surface becomes negatively charged, favoring the electrostatic adsorption of cationic dyes and promoting hole-driven oxidation near the semiconductor interface. Bicarbonate and carbonate can adsorb onto titania, forming (bi)carbonate surface species [
28]. However, under our conditions, the benefits of the strong SO-TiO
2 interaction outweigh this adsorption. Periodate continues to act as an efficient electron acceptor and photochemically activatable oxidant source (
•OH, IO
3•, IO
4•, etc.), so the ternary synergy that accelerates degradation remains largely intact despite bicarbonate buffering. Overall, the data suggest that at circum-alkaline pH, bicarbonate moderates, but does not impede, the performance of UV/TiO
2/IO
4−. Some 
•OH is converted to CO
3•−, and some sites are covered by (bi)carbonate. Nevertheless, SO adsorption at negatively charged TiO
2 and robust periodate-mediated charge separation maintain high removal rates.
 The apparent difference in pH between baseline conditions (6) and bicarbonate-containing systems (8.3) arises from the intrinsic buffering capacity of bicarbonate rather than from an imposed adjustment. Importantly, our previous study [
3] demonstrated that the degradation efficiency of the UV/TiO
2/IO
4− system is nearly identical at pH 6 and 8, confirming that this modest shift does not significantly influence photocatalytic performance. Within this range, TiO
2 exhibits a surface charge that is nearly neutral at pH 6 and slightly negative at pH 8.3, conditions that remain favorable for adsorption of the cationic dye. Periodate speciation is unaffected, with IO
4− prevailing as the dominant form.
Figure 8b illustrates the effect of nitrite on SO removal in the UV/TiO
2/IO
4− process. Nitrite causes strong, dose-dependent inhibition. There is a slight deceleration at concentrations of 0.1–1 mM, which becomes more pronounced at 10 mM and essentially stops the reaction at 100 mM. Three effects explain this trend. Nitrite reacts with 
•OH at a near-diffusion-controlled rate of k = 1.0 × 10
10 M
−1·s
−1 [
15], converting these potent oxidants into NO
2•. NO
2• is a moderate oxidant with an E° = 1.03 V/NHE, and it is far less effective toward many aromatics. The resulting drop in oxidative strength directly slows SO decay. Additionally, nitrite is readily oxidized at illuminated TiO
2 to nitrate and related intermediates. This consumes valence-band holes that would otherwise drive interfacial 
•OH formation and dye oxidation. Moreover, NO
2− absorbs in the 300–400 nm range (ε = 22 M
−1·cm
−1 at ~354–355 nm). At the studied concentration levels, this significantly reduces the number of photons that reach TiO
2 and periodate, thereby increasing kinetic losses. Although nitrite photolysis can generate 
•OH under UVA, the combined radical/hole scavenging and optical screening outweigh such production. This leads to the observed net inhibition. Since high activity in UV/TiO
2/IO
4− relies on periodate-assisted charge separation and multi-radical formation, nitrite emerges as a critical interferent.
 Overall, the kinetic limitations observed in saline matrices arise from two interrelated mechanisms. First, radical speciation shifts divert •OH into less reactive oxidants, with Cl− generating longer-lived chlorine radicals (Cl2•−/ClOH•−) and HCO3− producing CO3•−, thereby lowering the effective second-order reactivity toward SO. Second, interfacial and colloidal effects induced by elevated ionic strength and divalent cations (e.g., Ca2+, Mg2+) compress the electrical double layer, promote TiO2 aggregation, and enhance the adsorption of anions that block catalytic sites. Collectively, these pathways attenuate the periodate-assisted synergy that otherwise accelerates UV/TiO2/IO4− performance in low-salinity water.
  2.6. Surfactant Impact
The impact of non-ionic surfactants Triton X-100 and Tween 80 on SO degradation via UV/TiO
2/IO
4− process was shown in 
Figure 10a,b. The results clearly indicate that the presence of non-ionic surfactants consistently hinders the degradation of SO. The degree of inhibition increases with the amount of surfactant added. Without surfactants, SO is nearly depleted within 10 min. In contrast, after 30 min, a significant amount of residual SO remains when 10 mM of either Triton X-100 or Tween 80 is present. Intermediate concentrations (0.1–1 mM) produce graded, dose-dependent slowdowns. This behavior is expected for TiO
2 photocatalysis at pH 6 (near the point of zero charge of TiO
2), where efficient removal relies on access to photogenerated holes/
•OH and the electron acceptor periodate at the interface. Surface-active organics impede these pathways by occupying active sites and altering the interfacial microenvironment. Two concentration regimes explain these trends. Below or near the critical micelle concentration (CMC), individual surfactant molecules adsorb onto the TiO
2-water interface. There, they compete with SO and IO
4− for surface sites. This lowers the density of reactive centers and suppresses 
•OH formation and dye adsorption. Nonionic ethoxylates and polysorbates are known to adsorb appreciably onto TiO
2. The result is a modest but measurable kinetic penalty at 0.01 mM. Above the CMC, micellization dominates. SO partitions into the palisade/hydrophobic region of micelles, spatially separating the chromophore from the catalyst surface and reactive radicals. Concomitantly, micelles and surfactant layers can screen light and further reduce surface access. In micellar media, 
•OH radicals are less able to attack solutes buried within aggregates. This results in lower photocatalytic rates, a pattern also observed at 0.1–10 mM.
The contrasting CMCs of the two surfactants help explain the differences observed in the panels. The CMC of Triton X-100 in water ranges from 0.22 to 0.30 mM. In contrast, the CMC of Tween 80 ranges from 0.011 to 0.015 mM, about one order of magnitude lower. Consequently, 0.1 mM of Tween 80 is well above its CMC and strongly micellizing, while 0.1 mM of Triton X-100 remains below its CMC. At concentrations of 1–10 mM, both are well above their respective CMCs and strongly inhibitory. It should be noted that the CMC values referenced here are derived from measurements in pure water, whereas the actual micellization threshold may shift in the presence of TiO2, NaIO4, and at pH 6. In this study, the real CMC values under the experimental conditions were not quantified, and the discussion is therefore based on literature values as a conceptual framework. Given that ionic strength, divalent cations, and nanoparticle surfaces can influence micellization, future investigations should include direct CMC determinations in the relevant matrices to validate and refine the proposed interpretation. Typically, Tween 80 has a greater effect at equal molarity because it is deeper into the micellar regime.
Beyond sequestration and site blocking, chemical competition also contributes. Poly(ethylene oxide) chains and alkylphenol ethoxylates react rapidly with •OH and other oxidants. In the present photocatalytic AOP, the surfactants divert reactive species away from SO and the TiO2 surface, compounding the aforementioned physical effects.
Inhibition is particularly significant in the UV/TiO2/IO4− process because IO4− acts as an efficient electron acceptor that inhibits e−/h+ recombination. However, surfactant adsorption or micelle formation can reduce access of periodate to the catalyst surface. Consequently, electron scavenging becomes less effective, and the synergy of the ternary system diminishes. This is consistent with the observed convergence of the curves toward slower kinetics as the surfactant concentration increases.
When considered jointly, the data suggest that nonionic surfactants hinder SO degradation in three ways. First, they competitively adsorb onto TiO2, thereby blocking reactive sites. Second, at concentrations above the CMC, the surfactants sequester SO in micelles, limiting interfacial contact and radical attack. Third, they scavenge radicals with surfactant chains. To maintain the significant enhancement provided by periodate-assisted TiO2 photocatalysis, matrices containing detergents require one of the following strategies: a higher photon fluence or oxidant dose; pretreatment to remove surfactants; or methods to prevent interfacial fouling. These strategies include adsorptive pre-concentration, flow regimes that shear off soft layers, and catalyst modifications.